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dominated convergence theorem

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21: 18.2 General Orthogonal Polynomials
Markov’s theorem states that … This says roughly that the series (18.2.25) has the same pointwise convergence behavior as the same series with p n ( x ) = T n ( x ) , a Chebyshev polynomial of the first kind, see Table 18.3.1. … Part of this theorem was already proved by Blumenthal (1898). … See Szegő (1975, Theorem 7.2). …
22: 17.18 Methods of Computation
Method (1) is applicable within the circles of convergence of the defining series, although it is often cumbersome owing to slowness of convergence and/or severe cancellation. … Method (1) can sometimes be improved by application of convergence acceleration procedures; see §3.9. …
23: 10.74 Methods of Computation
In other circumstances the power series are prone to slow convergence and heavy numerical cancellation. … Newton’s rule is quadratically convergent and Halley’s rule is cubically convergent. … To ensure that no zeros are overlooked, standard tools are the phase principle and Rouché’s theorem; see §1.10(iv). …
24: 30.10 Series and Integrals
For an addition theorem, see Meixner and Schäfke (1954, p. 300) and King and Van Buren (1973). …
25: 10.44 Sums
§10.44(i) Multiplication Theorem
§10.44(ii) Addition Theorems
Neumann’s Addition Theorem
Graf’s and Gegenbauer’s Addition Theorems
26: 18.39 Applications in the Physical Sciences
An important, and perhaps unexpected, feature of the EOP’s is now pointed out by noting that for 1D Schrödinger operators, or equivalent Sturm-Liouville ODEs, having discrete spectra with L 2 eigenfunctions vanishing at the end points, in this case ± see Simon (2005c, Theorem 3.3, p. 35), such eigenfunctions satisfy the Sturm oscillation theorem. …Both satisfy Sturm’s theorem. …
See accompanying text
Figure 18.39.1: Graphs of the first and fourth excited state eigenfunctions of the harmonic oscillator, for = k = m = 1 , of (18.39.13), in ψ 1 ( x ) , ψ 4 ( x ) and those of the rational potential of (18.39.19), in ψ ^ 3 ( x ) , ψ ^ 6 ( x ) . Both sets satisfy the Sturm oscillation theorem. Magnify
Interactions between electrons, in many electron atoms, breaks this degeneracy as a function of l , but n still dominates. …
27: 1.5 Calculus of Two or More Variables
Implicit Function Theorem
§1.5(iii) Taylor’s Theorem; Maxima and Minima
§1.5(iv) Leibniz’s Theorem for Differentiation of Integrals
Suppose also that c d f ( x , y ) d y converges and c d ( f / x ) d y converges uniformly on a x b , that is, given any positive number ϵ , however small, we can find a number c 0 [ c , d ) that is independent of x and is such that … whenever both repeated integrals exist and at least one is absolutely convergent. …
28: 15.2 Definitions and Analytical Properties
On the circle of convergence, | z | = 1 , the Gauss series:
  • (a)

    Converges absolutely when ( c a b ) > 0 .

  • (b)

    Converges conditionally when 1 < ( c a b ) 0 and z = 1 is excluded.

  • 29: 16.2 Definition and Analytic Properties
    When p q the series (16.2.1) converges for all finite values of z and defines an entire function. … If none of the a j is a nonpositive integer, then the radius of convergence of the series (16.2.1) is 1 , and outside the open disk | z | < 1 the generalized hypergeometric function is defined by analytic continuation with respect to z . … On the circle | z | = 1 the series (16.2.1) is absolutely convergent if γ q > 0 , convergent except at z = 1 if 1 < γ q 0 , and divergent if γ q 1 , where …
    30: 18.33 Polynomials Orthogonal on the Unit Circle
    18.33.23 Φ n + 1 ( z ) = z Φ n ( z ) α n ¯ Φ n ( z ) ,
    Verblunsky’s Theorem
    Szegő’s Theorem
    For w ( z ) as in (18.33.19) (or more generally as the weight function of the absolutely continuous part of the measure μ in (18.33.17)) and with α n the Verblunsky coefficients in (18.33.23), (18.33.24), Szegő’s theorem states that …By (18.33.25) | α j | < 1 , so the infinite product in (18.33.31) converges, although the limit may be zero. …